394 research outputs found
The Twist of the Draped Interstellar Magnetic Field Ahead of the Heliopause: A Magnetic Reconnection Driven Rotational Discontinuity
Based on the difference between the orientation of the interstellar
and the solar magnetic fields, there was an expectation that the magnetic field
direction would rotate dramatically across the heliopause (HP). However, the
Voyager 1 spacecraft measured very little rotation across the HP. Previously we
showed that the twists as it approaches the HP and acquires a strong
T component (East-West). Here we establish that reconnection in the eastern
flank of the heliosphere is responsible for the twist. On the eastern flank the
solar magnetic field has twisted into the positive N direction and reconnects
with the Southward pointing component of the . Reconnection drives a
rotational discontinuity (RD) that twists the into the -T direction
and propagates upstream in the interstellar medium towards the nose. The
consequence is that the N component of is reduced in a finite width
band upstream of the HP. Voyager 1 currently measures angles
() close to solar values. We present MHD simulations
to support this scenario, suppressing reconnection in the nose region while
allowing it in the flanks, consistent with recent ideas about reconnection
suppression from diamagnetic drifts. The jump in plasma (the plasma to
magnetic pressure) across the nose of HP is much greater than in the flanks
because the heliosheath is greater there than in the flanks.
Large-scale reconnection is therefore suppressed in the nose but not at the
flanks. Simulation data suggest that will return to its pristine
value past the HP.Comment: 19 pages, 5 figures, submitte
Magnetohydrodynamic simulation of an equatorial dipolar paleomagnetosphere
Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/95191/1/jgra17407.pd
Magnetized jets driven by the sun: the structure of the heliosphere revisited
The classic accepted view of the heliosphere is a quiescent, comet-like shape
aligned in the direction of the Sun's travel through the interstellar medium
(ISM) extending for 1000's of AUs (AU: astronomical unit). Here we show, based
on magnetohydrodynamic (MHD) simulations, that the tension (hoop) force of the
twisted magnetic field of the sun confines the solar wind plasma beyond the
termination shock and drives jets to the North and South very much like
astrophysical jets. These jets are deflected into the tail region by the motion
of the Sun through the ISM similar to bent galactic jets moving through the
intergalactic medium. The interstellar wind blows the two jets into the tail
but is not strong enough to force the lobes into a single comet-like tail, as
happens to some astrophysical jets (Morsony et al. 2013). Instead, the
interstellar wind flows around the heliosphere and into equatorial region
between the two jets. As in some astrophysical jets that are kink unstable
(Porth et al. 2014) we show here that the heliospheric jets are turbulent (due
to large-scale MHD instabilities and reconnection) and strongly mix the solar
wind with the ISM beyond 400 AU. The resulting turbulence has important
implications for particle acceleration in the heliosphere. The two-lobe
structure is consistent with the energetic neutral atoms (ENAs) images of the
heliotail from IBEX (McComas et al. 2013) where two lobes are visible in the
North and South and the suggestion from the CASSINI (Krimigis et al. 2009,
Dialynas et al. 2013) ENAs that the heliosphere is "tailless".Comment: 19 pages, 5 figures; Astrophysical Journal Letters; in pres
Seasonal variation of aerosol water uptake and its impact on the direct radiative effect at Ny-Ålesund, Svalbard
© Author(s) 2014. This work is distributed under the Creative Commons Attribution 3.0 LicenseIn this study we investigated the impact of water uptake by aerosol particles in ambient atmosphere on their optical properties and their direct radiative effect (ADRE, W m-2) in the Arctic at Ny-Ålesund, Svalbard, during 2008. To achieve this, we combined three models, a hygroscopic growth model, a Mie model and a radiative transfer model, with an extensive set of observational data. We found that the seasonal variation of dry aerosol scattering coefficients showed minimum values during the summer season and the beginning of fall (July-August-September), when small particles (< 100 nm in diameter) dominate the aerosol number size distribution. The maximum scattering by dry particles was observed during the Arctic haze period (March-April-May) when the average size of the particles was larger. Considering the hygroscopic growth of aerosol particles in the ambient atmosphere had a significant impact on the aerosol scattering coefficients: the aerosol scattering coefficients were enhanced by on average a factor of 4.30 ± 2.26 (mean ± standard deviation), with lower values during the haze period (March-April-May) as compared to summer and fall. Hygroscopic growth of aerosol particles was found to cause 1.6 to 3.7 times more negative ADRE at the surface, with the smallest effect during the haze period (March-April-May) and the highest during late summer and beginning of fall (July-August-September).Peer reviewe
Constraining the pickup ion abundance and temperature through the multifluid reconstruction of the Voyager 2 termination shock crossing
Voyager 2 observations revealed that the hot solar wind ions (the so‐called pickup ions) play a dominant role in the thermodynamics of the termination shock and the heliosheath. The number density and temperature of this hot population, however, have remained unknown, since the plasma instrument on board Voyager 2 can only detect the colder thermal ion component. Here we show that due to the multifluid nature of the plasma, the fast magnetosonic mode splits into a low‐frequency fast mode and a high‐frequency fast mode. The coupling between the two fast modes results in a quasi‐stationary nonlinear wave mode, the “oscilliton,” which creates a large‐amplitude trailing wave train downstream of the thermal ion shock. By fitting multifluid shock wave solutions to the shock structure observed by Voyager 2, we are able to constrain both the abundance and the temperature of the undetected pickup ions. In our three‐fluid model, we take into account the nonnegligible partial pressure of suprathermal energetic electrons (0.022–1.5 MeV) observed by the Low‐Energy Charged Particle Experiment instrument on board Voyager 2. The best fitting simulation suggests a pickup ion abundance of 20 ± 3%, an upstream pickup ion temperature of 13.4 ± 2 MK, and a hot electron population with an apparent temperature of ~0.83 MK. We conclude that the actual shock transition is a subcritical dispersive shock wave with low Mach number and high plasma β.Key PointsFirst multifluid MHD reconstruction of the termination shockThe termination shock is a high‐β low–Mach number dispersive shock waveObservational constraint on the pickup ion abundance and temperaturePeer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/116003/1/jgra52059_am.pdfhttp://deepblue.lib.umich.edu/bitstream/2027.42/116003/2/jgra52059.pd
Hydrogen-induced ferromagnetism in ZnO single crystals investigated by Magnetotransport
We investigated the electrical and magnetic properties of low-energy
hydrogen-implanted ZnO single crystals with hydrogen concentrations up to 3
at.% in the first 20 nm surface layer between 10 K and 300 K. All samples
showed clear ferromagnetic hysteresis loops at 300 K with a saturation
magnetization up to 4 emu/g. The measured anomalous Hall effect agrees with the
hysteresis loops measured by superconducting quantum interferometer device
magnetometry. All the H-treated ZnO crystals exhibited a negative
magnetoresistance up to the room temperature. The relative magnitude of the
anisotropic magnetoresistance reaches 0.4 % at 250 K and 2 % at 10 K,
exhibiting an anomalous, non-monotonous behavior and a change of sign below 100
K. All the experimental data indicate that hydrogen atoms alone in a few
percent range trigger a magnetic order in a ZnO crystalline state. Hydrogen
implantation turns out to be a simpler and effective method to generate a
magnetic order in ZnO, which provides interesting possibilities for future
applications due to the strong reduction of the electrical resistance
The Phylogeography of Rabies in Grenada, West Indies, and Implications for Control
In Grenada, West Indies, rabies is endemic, and is thought to be maintained in a wildlife host, the small Indian mongoose (Herpestes auropunctatus) with occasional spillover into other hosts. Therefore, the present study was undertaken to improve understanding of rabies epidemiology in Grenada and to inform rabies control policy. Mongooses were trapped island-wide between April 2011 and March 2013 and examined for the presence of Rabies virus (RABV) antigen using the direct fluorescent antibody test (dFAT) and PCR, and for serum neutralizing antibodies (SNA) using the fluorescent antibody virus neutralization test (FAVN). An additional cohort of brain samples from clinical rabies suspects submitted between April 2011 and March 2014 were also investigated for the presence of virus. Two of the 171 (1.7%) live-trapped mongooses were RABV positive by FAT and PCR, and 20 (11.7%) had SNAs. Rabies was diagnosed in 31 of the submitted animals with suspicious clinical signs: 16 mongooses, 12 dogs, 2 cats and 1 goat. Our investigation has revealed that rabies infection spread from the northeast to the southwest of Grenada within the study period. Phylogenetic analysis revealed that the viruses from Grenada formed a monophyletic clade within the cosmopolitan lineage with a common ancestor predicted to have occurred recently (6–23 years ago), and are distinct from those found in Cuba and Puerto Rico, where mongoose rabies is also endemic. These data suggest that it is likely that this specific strain of RABV was imported from European regions rather than the Americas. These data contribute essential information for any potential rabies control program in Grenada and demonstrate the importance of a sound evidence base for planning interventions
Probing IMF using nanodust measurements from inside Saturn's magnetosphere
We present a new concept of monitoring the interplanetary magnetic field (IMF) by using in situ measurements of nanodust stream particles in Saturn's magnetosphere. We show that the nanodust detection pattern obtained inside the magnetosphere resembles those observed in interplanetary space and is associated with the solar wind compression regions. Our dust dynamics model reproduces the observed nanodust dynamical properties as well as the detection pattern, suggesting that the ejected stream particles can reenter Saturn's magnetosphere at certain occasions due to the dynamical influence from the time‐varying IMF. This method provides information on the IMF direction and a rough estimation on the solar wind compression arrival time at Saturn. Such information can be useful for studies related to the solar wind‐magnetosphere interactions, especially when the solar wind parameters are not directly available. Key Points A new method to probe IMF with nanodust measurements inside the magnetosphere Under changing IMF, ejected nanoparticles can re‐enter Saturn‐s magnetosphere IMF direction and solar wind compression arrival time can be derivedPeer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/99078/1/grl50604.pd
Deeply Virtual Compton Scattering
We study in QCD the physics of deeply-virtual Compton scattering (DVCS)---the
virtual Compton process in the large s and small t kinematic region. We show
that DVCS can probe a new type of off-forward parton distributions. We derive
an Altarelli-Parisi type of evolution equations for these distributions. We
also derive their sum rules in terms of nucleon form-factors of the twist-two
quark and gluon operators. In particular, we find that the second sum rule is
related to fractions of the nucleon spin carried separately by quarks and
gluons. We estimate the cross section for DVCS and compare it with the
accompanying Bethe-Heitler process at CEBAF and HERMES kinematics.Comment: 20 pages, 2 figures, replaced with the version to appear in Phys.
Rev.
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